Aspects of the present disclosure describe techniques that involve an active stabilization of coherent controllers using nearby qubits. In an aspect, a quantum information processing (QIP) system for stabilizing phase damping in qubits is described that provides a first and a second qubit ion, measuring magnetic field fluctuations using the second qubit ion, and generates one or more magnetic fields based on the measured magnetic field fluctuations, the one or more magnetic fields being applied near the first qubit ion to cancel the magnetic field fluctuations to stabilize the phase damping of the first qubit ion. Another such QIP system performs provides a first and a second qubit ion, locks a local oscillator to a frequency reference associated with the second qubit ion, and tracks, using the local oscillator, a frequency of the first qubit ion based on the frequency reference. Methods associated with these QIP systems are also described.
Legal claims defining the scope of protection, as filed with the USPTO.
1. A trapped ion quantum information processing (QIP) system, comprising: at least one ion trap having at least one first qubit ion and at least one second qubit ion; one or more coils; and a stabilizer for stabilizing phase damping in qubits, the stabilizer being configured to: measure magnetic field fluctuations using the at least one second qubit ion; and generate, using the one or more coils, one or more magnetic fields based on the measured magnetic field fluctuations, the one or more magnetic fields being applied near the at least one first qubit ion to cancel the magnetic field fluctuations to stabilize the phase damping of the at least one first qubit ion.
2. The QIP system of claim 1, wherein: the at least one first qubit ion includes a plurality of first qubit ions, the at least one second qubit ion includes a plurality of second qubit ions, or the at least one first qubit ion includes a plurality of first qubit ions and the at least one second qubit ion includes a plurality of second qubit ions.
3. The QIP system of claim 1, wherein the phase damping is characterized by a measurement of a parameter T2.
4. The QIP system of claim 1, wherein the at least one first qubit ion and the at least one second qubit ion are atomic hyperfine qubits.
5. The QIP system of claim 4, wherein the at least one first qubit ion is addressable with a first wavelength of light and the at least one second qubit ion is addressable with a second wavelength of light different from the first wavelength of light.
6. The QIP system of claim 5, wherein the at least one first qubit ion is a qubit made from 171Yb+ and the at least one second qubit ion is a qubit made from 133Ba+.
7. The QIP system of claim 1, wherein: the at least one ion trap includes a single ion trap, and the at least one first qubit and the at least one second qubit are co-trapped in the single ion trap.
8. The QIP system of claim 1, wherein: the at least one ion trap includes a first ion trap and a second ion trap nearby the first ion trap, and the at least one first qubit is trapped in the first ion trap and the at least one second qubit is trapped in the second ion trap.
9. The QIP system of claim 1, wherein: the at least one second qubit ion has energy levels that are sensitive to magnetic fields, and the stabilizer is configured to measure the magnetic field fluctuations using the energy levels of the at least one second qubit ion that are sensitive to magnetic fields.
10. The QIP system of claim 9, wherein the at least one second qubit ion has other energy levels that are insensitive to magnetic fields.
11. The QIP system of claim 9, wherein the energy levels that are sensitive to magnetic fields include Zeeman levels.
12. The QIP system of claim 1, wherein the magnetic field fluctuations include 60 Hz noise.
13. The QIP system of claim 1, further comprising a magnetic shield configured to reduce the magnetic field fluctuations near the at least one first qubit ion and the at least one second qubit ion, wherein the magnetic shield is made of a material with high magnetic permeability including one or more of mu-metal, highly conductive copper, or a superconducting material at cryogenic temperatures.
14. The QIP system of claim 1, wherein the stabilizer is configured to repeat, as part of a feedback loop, a sequence that includes the measuring of the magnetic field fluctuations and the generation of the one or more magnetic fields to cancel the magnetic field fluctuations.
15. The QIP system of claim 14, wherein the feedback loop has a bandwidth of at least 1 KHz.
16. The QIP system to claim 1, wherein the stabilizer is configured to measure the magnetic field fluctuations using the at least one second qubit ion by being further configured to optically probe energy levels of the at least one second qubit ion that are sensitive to magnetic fields to detect characteristics of the magnetic field fluctuations.
17. The QIP system of claim 1, wherein: the QIP system is configured to perform a quantum computation, the at least one first qubit ion is configured to participate in the quantum computation, and the at least one second qubit ion is a spectator qubit that is not configured to participate in the quantum computation.
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June 29, 2021
April 29, 2025
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